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Exterior exhaustion bounds for normalized Schrödinger solutions

Statement

On a connected exterior as in the exterior-data definition, let V≥0 be smooth and let u∈C2(Σ∘)∩Cloc1(Σ) solve (Δh−V)u=0, vanish on S, and tend uniformly to c>0 as r→∞. Then 0<u≤c in the interior. If S is nonempty, then u<c there.

Facts & Assumptions

Given: The end chart and compact core are those of Weighted exterior elliptic domains and admissible weights. The limit means that for every ϵ>0, ∣u−c∣<ϵ beyond a sufficiently large end sphere. Use compact comparison Compact-domain comparison with a nonnegative potential and the strong minimum alternative Strong minimum principle from the annular barrier.

Proof

Given: The hypotheses and data in the Statement and Facts & Assumptions.

Goal: Establish the conclusions of the Statement.

Proof technique: direct.

1.1given

Truncate the exterior at r=R. For R sufficiently large, u≥c/2>0 on the outer sphere and u=0 on S. Comparison applied to −u gives u≥0 on the truncation. Applied to u−(c+ϵ), whose image under Δh−V is V(c+ϵ)≥0, it gives u≤c+ϵ when the outer sphere satisfies that bound. Every fixed point belongs to all sufficiently large truncations. Taking R large and then ϵ↓0 proves 0≤u≤c. Components of a truncation meet its boundary; otherwise such a component would be a compact component of the connected exterior separated from its end.

2.1step 1.1givenalgebra∎

The end limit excludes u≡0, so the strong minimum alternative makes u>0. The nonnegative function c−u satisfies (Δh−V)(c−u)=−Vc≤0. If it vanished inside, the same alternative would make u≡c. This contradicts u∣S=0 when S≠∅. Thus the stated strict upper bound also holds.

Depends on

Used by · 1

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